Methods for Determining a Position of a Droppable Object in a Wellbore

Abstract

The position of a droppable object (e.g., a cementing plug or drillpipe dart) in a cased wellbore may be determined in real time during a cementing operation. A pressure data acquisition system is installed at a wellsite and a pressure transducer is installed at the wellhead. As the droppable object travels through casing it encounters regions with a positive or a negative change of inner cross-sectional dimension. The droppable object generates a pressure pulse as it passes through the regions. The pressure pulse and associated reflections are detected by the pressure transducer, and the signals are processed mathematically to determine the current position of the droppable object.

Claims

1. A method for determining a position of a droppable object inside a casing string, comprising: (i) installing the casing string into a liquid filled borehole, wherein the casing string comprises at least one region with a negative or a positive change of inner cross-sectional dimension; (ii) installing a pressure data acquisition system at a wellsite, and a pressure transducer at a wellhead; (iii) placing the droppable object inside the casing string; (iv) pumping a fluid behind the droppable object, causing the droppable object to travel through the interior of the casing string and pass through the at least one region with a negative or a positive change of inner cross-sectional dimension, thereby generating a pressure pulse; (v) recording the pressure data with a pressure transducer, and transmitting the pressure data to the pressure data acquisition system; and (vi) processing the pressure data mathematically by obtaining the pressure pulses, pulse reflections or both, and determining the position of the droppable object.

2. The method of claim 1, wherein the droppable object is a top cementing plug, or a bottom cementing plug, or a drill pipe dart.

3. The method of claim 1, wherein the change of inner cross-sectional dimension is located at casing pipe joints, wherein the casing pipe joints comprise screw joints, weld joints or both.

4. (canceled)

5. The method of claim 1, wherein the mathematical processing of the pressure pulses and pulse reflections comprises cepstral analysis, comprising producing a pressure cepstrogram in coordinates of quefrency and time, and calculating the pressure pulse reflection time from the droppable object traveling through the casing string.

6. The method of claim 1, wherein the mathematical processing further comprises determination of a tube wave velocity, based on the pressure pulse reflection time from a stationary object with a known position in the wellbore.

7. The method of claim 1, where the reflection time from the droppable object is converted to the position of droppable object by multiplication by tube wave velocity.

8. The method of claim 1, wherein the mathematical processing comprises analyzing a pressure spectrogram and determination of pressure pulses.

9. The method of claim 1, wherein the mathematical processing comprises analyzing a normalized energy spectral density of the pressure data.

10. The method of claim 9, wherein the normalized energy spectral density is computed by integrating the pressure spectrogram along the frequency axis followed by normalization.

11. The method of claim 1, wherein the mathematical processing comprises a correlation between anticipated pressure pulses based on casing tally information and pressure pulses from the pressure spectrogram or normalized energy spectral density.

12. The method of claim 1, wherein the locating of the droppable object is performed in real time during pumping, allowing an operator to control movement of the droppable object.

13. (canceled)

14. A method for cementing a borehole penetrating a subterranean formation, comprising: (i) installing a casing string into the is liquid-filled borehole, wherein the casing string comprises at least one region with a negative or a positive change of inner cross-sectional dimension; (ii) installing a pressure data acquisition system at a wellsite, and at least one pressure transducer at a wellhead; (iii) placing a top cementing plug inside the casing string; (iv) pumping a displacement fluid behind the top cementing plug, causing the top cementing plug to travel through the interior of the casing string and pass through the at least one region with a negative or a positive change of inner cross-sectional dimension, thereby generating a pressure pulse; (v) using the at least one pressure transducer to detect the pressure pulse and transmit pressure data to the pressure data acquisition system, the pressure data comprising pressure pulse propagation velocity and reflection time; and (vi) processing the pressure data mathematically and determining the position of the top cementing plug.

15. The method of claim 14, further comprising: (a) placing a bottom cementing plug inside the casing string; (b) pumping a cement slurry behind the bottom cementing plug, causing the bottom cementing plug to travel through the interior of the casing string and pass through the at least one region with a negative or a positive change of inner cross-sectional dimension, thereby generating a pressure pulse; (c) using the at least one pressure transducer to detect the pressure pulse and transmit pressure data to the pressure data acquisition system, the pressure data comprising a pressure pulse propagation velocity and a reflection time; and (d) processing the pressure data mathematically and determining the position of the bottom cementing plug.

16. (canceled)

17. The method of claim 14, wherein the mathematical processing comprises cepstral analysis, comprising producing a pressure cepstrogram in coordinates of quefrency and time, and calculating the pressure pulse reflection time from the top or bottom wiper plug.

18. The method of claim 14, wherein the mathematical processing further comprises determination of tube wave velocity, based on reflection time from a stationary object with a known position in the wellbore.

19. The method of claim 14, wherein reflection time from the top cementing plug is converted to the position of the top cementing plug by multiplication by tube wave velocity.

20. The method of claim 14, wherein the mathematical processing comprises analyzing a pressure spectrogram and determination of pressure pulses.

21. The method of claim 14, wherein the mathematical processing comprises analyzing a normalized energy spectral density of the pressure data.

22. The method of claim 14, wherein the normalized energy spectral density is computed by integrating the pressure spectrogram along the frequency axis followed by normalization.

23. The method of claim 14, wherein the mathematical processing comprises a correlation between anticipated pressure pulses based on casing tally information and pressure pulses from the pressure spectrogram or normalized energy spectral density.

24. The method of claim 14, wherein the locating of the cementing plug is performed in real time during pumping, allowing an operator to make instant decisions concerning treatment progress.

25. The method of claim 14, wherein the velocity of tube wave propagation is taken from measurements recorded while cementing a previous section or a neighbouring well with similar characteristics.

Description

BRIEF DESCRIPTION OF THE DRAWINGS

[0012] FIG. 1 shows a typical wellsite configuration during a cementing operation.

[0013] FIG. 2 shows a cementing operation in progress. The bottom cementing plug has been released, separating the cement slurry from chemical washes, spacer fluids and drilling fluid.

[0014] FIG. 3 shows a cementing operation in progress. The bottom cementing plug has landed on the float collar. A membrane in the bottom cementing plug ruptures, allowing cement slurry to enter the annulus between the casing string and the borehole wall.

[0015] FIG. 4 shows a completed cementing operation. Cement slurry fills the annulus, both cementing plugs have landed on the float collar, and the interior of the casing string is filled with displacement fluid.

[0016] FIG. 5 is an illustration of a cementing plug passing through a region of casing pipe with a negative and a positive change of inner cross-sectional dimension.

[0017] FIG. 6 is an illustration of a cementing plug passing through a casing joint with an inner cross-sectional dimension di, which is different from the rest of the casing dz.

[0018] FIG. 7 is an illustration of a well configuration for practicing the disclosed methods.

[0019] FIGS. 8(i) and 8(ii) show the computation workflow for determining pressure pulses arising from cementing plugs passing through casing collars. FIG. 8(i)(a) is a plot of wellhead pressure and flowrate versus time; FIG. 8(i)(b) shows the wellhead pressure spectrogram; FIG. 8(ii)(c) shows the normalized energy spectral density; FIG. 8(ii)(d) is a plot of displaced volume and estimated cementing plug depth versus time; FIG. 8(ii)(e) is a plot of measured pressure pulses arising from the cementing plug passing through casing collars.

[0020] FIG. 9 shows the depths associated with each pressure pulse, according to the casing tally.

[0021] FIG. 10 shows pressure pulses according to a casing tally when casing joints of non-uniform spacing are present.

[0022] FIG. 11 shows example data from a primary cementing operation: pressure at the wellhead, frequency-time diagram and reflective signal intensity.

[0023] FIG. 12 shows example data from a primary cementing operation: reflective signal intensity diagram and pressure evolution at the wellhead.

SUMMARY

[0024] In an aspect, embodiments relate to methods for determining a position of a droppable object inside a casing string. A casing string is installed in a wellbore, during which a fluid medium in the borehole enters and fills the interior of the casing string. The casing string comprises at least one region with a negative or a positive change of inner cross-sectional dimension. A pressure data acquisition system is installed at the wellsite, and a pressure transducer is installed at the wellhead.

[0025] A droppable object is then placed inside the casing string. The droppable object may be a top cementing plug, a bottom cementing plug or a drill pipe dart. A fluid is then pumped behind the droppable object, causing the droppable object to travel through the interior of the casing string and pass through the at least one region with a negative or positive change of inner cross-sectional dimension, thereby generating a pressure pulse.

[0026] The pressure data are recorded by the pressure transducer and transmitted to the pressure data acquisition system. The pressure data are then processed mathematically by obtaining the pressure pulses, pulse reflections or both, and the position of the droppable object is determined.

[0027] In a further aspect, embodiments relate to methods for cementing a borehole penetrating a subterranean formation. A casing string is installed into the liquid-filled borehole, during which drilling fluid in the borehole enters and fills an interior of the casing string, wherein the casing string comprises at least one region with a negative or a positive change of inner cross-sectional dimension. A pressure data acquisition system is installed at the wellsite, and a pressure transducer is installed at the wellhead.

[0028] The pressure transducer is used to detect the pressure pulse and pulse reflections, and transmit pressure data to the pressure data acquisition system. The pressure data are then processed mathematically and the position of the bottom cementing plug is determined.

[0029] A top cementing plug is placed inside the casing string. A displacement fluid is pumped behind the top cementing plug, causing the top cementing plug to travel through the interior of the casing string and pass through the at least one region with a negative or a positive change or inner cross-sectional dimension, thereby generating a pressure pulse.

[0030] The at least one pressure transducer is used to detect the pressure pulses, pulse reflections or both, and transmit the pressure data to the pressure data acquisition system. The pressure data are then processed mathematically and the position of the top cementing plug is determined.

DETAILED DESCRIPTION

[0031] At the outset, it should be noted that in the development of any such actual embodiment, numerous implementationsspecific decisions must be made to achieve the developer's specific goals, such as compliance with system related and business related constraints, which will vary from one implementation to another. Moreover, it will be appreciated that such a development effort might be complex and time consuming but would nevertheless be a routine undertaking for those of ordinary skill in the art having the benefit of this disclosure. In addition, the composition used/disclosed herein can also comprise some components other than those cited. In the summary of the disclosure and this detailed description, each numerical value should be read once as modified by the term about (unless already expressly so modified), and then read again as not so modified unless otherwise indicated in context. Also, in the summary of the disclosure and this detailed description, it should be understood that a concentration range listed or described as being useful, suitable, or the like, is intended that any and every concentration within the range, including the end points, is to be considered as having been stated. For example, a range of from 1 to 10 is to be read as indicating each and every possible number along the continuum between about 1 and about 10. Thus, even if specific data points within the range, or even no data points within the range, are explicitly identified or refer to only a few specific points, it is to be understood that inventors appreciate and understand that any and all data points within the range are to be considered to have been specified, and that inventors possessed knowledge of the entire range and all points within the range.

[0032] This disclosure pertains to detecting the position of droppable objects in a casing string or liner during a well cementing operation. The droppable objects may comprise top or bottom cementing plugs and drill pipe darts. The method is based on generating pressure pulses in a well, recording high frequency pressure data, mathematical processing of the recorded data with extraction of pressure pulses and pressure pulses reflections from downhole objects, measuring the pulse reflection times and computing the distance from a known position of the pressure transducer to the droppable object. The methods and measurements disclosed herein may be performed in real time during a cementing operation. The ability to locate droppable objects in real time allows operators to make instant decisions concerning the progress of the treatment, for example, whether to continue or discontinue displacement, volumes of fluids to be introduced into the wellbore and pumping rates.

[0033] A method and system for locating steady downhole objects that reflect a hydraulic signal are disclosed in the patent application WO 2018/004369. The monitoring of the well is based on cepstral analysis of pressure data recorded at the wellhead. It is designed to locate steady downhole objects that reflect a hydraulic signal. A hydraulic signal is detected by a pressure sensor, then the pressure data are processed to obtain their properties such as tube wave reflection times. One (but not the only) method of obtaining such information is a cepstrum analysis. The cepstrum analysis is widely used in various applications, for example for hydraulic fracturing operations monitoring. The cepstrogram allows detection of objects that reflect the hydraulic signal. This method for hydraulic fracturing operations uses hydraulic signal sources including the water hammer effect, noise from surface or submersible pumps and perforating events.

[0034] U.S. Pat. No. 6,401,814 B1 discloses a method for locating a cementing plug in a subterranean well during cementing operations using pressure pulse reflections. Once generated, pressure pulses are transmitted through displacement fluid, reflected off the cementing plug and, finally, received by a pressure sensor. A location of the plug is calculated from reflection time and pressure pulse velocity in the given media. The method of generating and transmitting of pressure pulse through the fluid in a casing string comprises momentarily opening a valve installed in the flowline of the well. Other methods of pressure pulse generation include an air gun, varying the pump's engine speed or disengaging the pump.

[0035] U.S. Pat. No. 5,754,495 discloses a method for acoustic determination of the length of a fluid conduit. It comprises constructing a pressure containment system, connecting pressure sensors, filling the system with a fluid, generating a pressure pulse, measuring a pressure pulse traveling to the distal end of the fluid conduit, and calculating the length of the fluid conduct. In the embodiment, a tube wave is generated by a sudden release of pressure in the well through a valve.

[0036] U.S. Pat. No. 4,819,726 discloses a method for indicating the position of a cement wiper plug prior to its bottomhole arrival. It comprises an apparatus that includes a section of pipe string with an interior shearable, temporary means of restricting the motion of the cement wiper plug through the section of pipe string. The arrival of the cementing plug at the shearable, temporary restriction means in a pipe string is sensed by an increase in pipe string pressure at the surface and monitored by a pressure sensor.

[0037] U.S. Pat. No. 9,546,548 discloses a device and a method of use for cement sheath analysis based on acoustic wave propagation. It consists of an acoustic wave detection apparatus, comprising a fiber optic cable drawn down in a well, an optical source and a data acquisition system. The acoustic source produces a compressional wave in a casing string. The pressure in the annulus is determined as the cement slurry sets, and this pressure is compared to the maximum formation pressure as an indication of whether the cement had set to a strength, enough to maintain an effective formation-to-casing seal across the annulus.

[0038] In the methods disclosed in this application, pressure pulses are generated when a cementing plug passes through casing collar joints where a variation of inner diameter of the casing takes place. Computation of the distance is based on determining the velocity of tube waves generated by the pressure pulses, and the travel time of the tube wave between the pressure transducer and the droppable object. Reflection times are obtained through the cepstrum analysis of recorded high frequency pressure data. As described in patent application WO 2018/004369 referenced above, a cepstrum is the result of taking the inverse Fourier transform (IFT) of the logarithm of the estimated spectrum of a signal. Tube wave velocity may be obtained using computed pressure pulse reflection time from the objects in wellbore with a known position, for example a landing collar, or calculated theoretically based on parameters including properties of the liquid medium and the casing geometry. Another embodiment utilizes the identification of wiper plug position based on pressure pulse generation and the information about the casing joint sequencecalled a casing tally. It comprises pressure pulse generation by the wiper plug passing through the collar, its detection and matching with its depth taken from the casing tally table.

[0039] One embodiment of the disclosure is a system that comprises at least two casing pipes joined together to form a casing string and placed in the borehole (FIG. 5). A cementing plug 107 is dropped into a casing string 103 filled with a fluid. At least one pipe in the casing string may have a region with at least one change of inner cross-section dimension. The change of inner cross-section dimension can be negative 501 or positive 502 with respect to the inner cross- sectional dimension of the rest of the pipe. The change of inner cross-sectional dimension may occur at casing pipe joints, which may be screw joints 601, weld joints or both (FIG. 6). A pressure pulse is generated when the cementing plug passes through the region with the change of inner cross-sectional dimension (501, 502, or 601) due to the difference in forces (602, 603) required to push the cementing plug through the region d.sub.1 and the rest of the pipe d.sub.2. The change of inner cross-sectional dimension may further be a restriction, a groove, a lug, or an orifice or a combination thereof. Furthermore, the distances between regions with at least one change of inner cross-sectional dimension may be equidistant or nonequidistant, or both.

[0040] The disclosed method employs an assembly (FIG. 7) that comprises a borehole 102, fluid-filled casing string run into borehole 103, a pressure transducer 701 installed at the casing string at the surface (wellhead or cementing head), an acquisition system 702 for pressure data recording, and at least one pump 703 connected to the casing string via the cementing head 101. The pressure transducer may be installed at a fluid pumping line, for example at the cementing head. Or, the pressure transducer may be installed at the annular side of the casing (e.g., at a blowout preventer). The pressure pulses may be recorded within a frequency range between 20 and 2000 Hz. Once generated, a pressure pulse 704 may propagate in the fluid-filled borehole and reflect from various objects. The pulse reflection objects are any physical or geometrical changes in the borehole and casing string, that may include, but not limited to a droppable objects such as a cementing plug 107, top of cement and fluid interfaces, or stationary objects such as a landing collar 705, a liner, a check valve, a bottomhole 706, fractures and vugs. Pulse propagation and reflection may occur several times until they completely attenuate. Pulse reflections from various objects are detected by the pressure transducer installed at the surface and data are captured by the acquisition system. Recorded pressure data are then processed with a mathematical algorithm and reflection times from various objects are obtained. The mathematical algorithm may be cepstral analysis, comprising production of a pressure cepstrogram in coordinates of quefrency and time, and calculation of pressure pulse reflection time from the droppable object. The location of the object relatively to known position of pressure transducer is then calculated by multiplication of the reflection half-time by the velocity of pulse propagation in the media filling the volume between the pressure transducer and the object. The reflection time from the droppable object may be converted to the position of the droppable object by multiplication by tube wave velocity.

[0041] Persons skilled in the art will recognize that the disclosed methods may further comprise placing a bottom cementing plug inside the casing string. Cement slurry may be pumped behind the bottom cementing plug. The bottom cementing plug may travel through the interior of the casing string and pass through at least one region with a negative or a positive change of inner cross-sectional dimension, thereby generating a pressure pulse. The at least one pressure transducer may be used to detect the pressure pulse and transmit pressure data to the pressure data acquisition system. The pressure data may be processed mathematically and the position of the bottom cementing plug may be determined. Monitoring of the bottom cementing plug may proceed at least until the top cementing plug is launched.

[0042] In one another embodiment the velocity of pressure pulse propagation in the media is taken from measurements while cementing a previous section or a neighboring well with similar characteristics.

[0043] Locating the object may be performed in real time during the cementing operation. It is implemented via recording and mathematical processing of the pressure signal followed by object positioning directly during the cementing operation. A computer with specific software may perform immediate data processing and building a tracking diagram of the object.

[0044] Another embodiment uses information about the casing joint sequence called the casing tally. The casing tally is a table that stores the lengths and positions of all casing collars. The pulse generated by the cementing plug passing a collar can be matched with its depth taken from the casing tally table as illustrated in FIGS. 8(i), 8(ii) and 9.

[0045] The high frequency pressure and pump rate are shown in FIG. 8(i)(a). The spectrogram of the pressure signal is a visual representation of the spectrum of frequencies of the signal as it varies with time, shown in FIG. 8(ii)(b). Although the pressure pulses are not recognizable on the pressure curve they are clearly seen on the spectrogram as broadband events. Furthermore, these pulses manifest themselves as peaks on the normalized energy spectral density plot shown in FIG. 8(ii)(c).

[0046] Energy spectral density describes how the energy of a signal is distributed with frequency. The term energy is used in the generalized sense of signal processing; that is, the energy E of a signal x(t) is:

E=.sub..sup.|x(t).sup.2|dt (1)

[0047] The energy spectral density is most suitable for transients(e.g.) pulse-like pressure signalshaving a finite total energy. In this case, Parseval's theorem provides an alternate expression for the energy of the signal:

.sub..sup.|x(t).sup.2|dt =.sub..sup.|{circumflex over (x)}(f)|.sup.2df (2)

where

x(f)=.sub..sup.e.sup.2iftx(t)dt (3)

is the Fourier transform of the signal and f is the frequency in Hz. Often used is the angular frequency =2f. Since the integral on the right-hand side is the energy of the signal, the integrand |{circumflex over (x)}(f)|.sup.2can be interpreted as a density function describing the energy per unit frequency f. In light of this, the energy spectral density of a signal x(t) is defined as

S.sub.xx(f)=|{circumflex over (x)}(f)|.sup.2. (4)

[0048] The normalized energy spectral density is computed by integrating the spectrogram along the frequency axis followed by normalization by the strongest peak. The normalized energy spectral density is therefore a dimensionless quantity. From FIG. 8(ii)(c) it is also shown that the time interval between these peaks depends on the pump rate. The time interval is shorter at the pump rate of 1 m.sup.3/min and longer at the pump rate of [0.5 m.sup.3/min (3.1 bbl/min)]. A convenient way to correct for a non-constant pump rate is to convert the time scale to the estimated depth scale as shown in FIG. 8(ii)(d). By integrating the pump rate over time, the displaced volume curve may be computed. The displaced volume scale in reverse order is shown on the left y-axis of FIG. 8(ii)(d). Taking into account the inner casing diameter, the estimated depth scale may be computed as shown by the right y-axis of FIG. 8(ii)(d). The horizontal time scale from FIG. 8(ii)(c) is mapped with the displaced volume curve to determine the estimated cementing plug depth. The normalized energy spectral density information may be plotted against estimated depth scale to produce a collar pulses plot, shown in FIG. 8(ii)(e).

[0049] As shown in FIG. 9, the collar pulses plot from FIG. 8(ii)(e) may then be compared with a known casing tally to determine the depth of the cementing plug. Persons skilled in the art will recognize that the position of the bottom plug may be monitored during the period before the top plug is launched.

[0050] The workflow described above functions optimally when all of the pulses are clearly seen on the normalized energy spectral density plot. In some cases, the amplitude of one or more pulses may be too low due to tube wave attenuation in the wellbore, or buried with the noise or both. Also, due to the U-tubing effect, the pressure pulses may not be immediately visible after a plug is released from the cementing head, but after the cementing plug has traveled to some depth from the surface. In this case, if all joints have the same length matching anticipated pulses with the measured ones may be ambiguous. This circumstance may be avoided by installing casing segments at various locations that are shorter or longer than the normal sequence. In other words, the distances between regions with at least one change of inner cross-sectional dimension may be equidistant or non-equidistant. This way, the casing tally should contain one or more shorter or longer joints or their combination so that they can be clearly seen on the measured pulses plot. These pulses would then be used as a benchmark for correlation between anticipated pressure pulses with the casing tally as the collars number K and K+1 shown in FIG. 10.

EXAMPLE

[0051] The following example serves to further illustrate the disclosure.

[0052] In the practical example of current invention, a pressure transducer was installed at a cementing head of the wellbore with 34-cm (13- inch) casing having a true vertical depth of 600 m (1969 ft) and a landing collar at a depth of 585 m (1919 ft). The well was cemented by pumping cement slurry followed by oil-base displacement fluid. Two cementing plugs, bottom and top, were used to prevent contamination of the cement slurry. The pressure at cementing head was recorded with the rate of 500 pints per second using a Viatran 509 pressure transducer and acquisition device. The recorded data were then processed by cepstrum analysis, and the reflection times of pressure pulses from various objects were obtained. The top cementing plug was tracked by means of the disclosed method. FIG. 11 shows the results of the high frequency pressure data processing by cepstral analysis and includes a pressure profile (a), frequency (b), and reflective signal intensity diagram (c) with pressure pulse reflection time from wiper plug versus cement displacement job time. From diagram (b) one can see periodic (every 50 s) broadband signals 1101 corresponding to pressure pulses generated by the cementing plug passing through joints of casing pipes with a positive change of inner cross-sectional dimension (local enlargement) after every 10.5 m (34.4 ft) of the tubular element. Taking into account known parameters provided by the cementing job report, such as the pumping rate [1.02 m.sup.3 (6.4 bbl/min)], casing inner diameter [31.7 cm (12.475 inch)] and the distance between two joints [10.5 m (34.4 ft)], one may calculate that the cementing plug passes a casing joint every 52 s, which is in agreement with the 50 s period of pulses 1101 on the frequency diagram (b). Moreover, when the pumping rate was decreased to [0.48 m.sup.3 (3 bbl/min)] after 1650 s of the job, the cementing plug velocity decreased and the time to travel between two casing joints was 116 s. At the same time, the period of pulses 1102 observed in the diagram (b) increased to 110 s. These primary pulses may be correlated with the casing tally for determining plug position during displacement. Further, the pulses generated by the cementing plug passing through casing joints propagate along the wellbore to the cementing head, and some reflect back and forth until they attenuate completely. On the reflective signal intensity diagram (c) the line 1103 that corresponds to the pressure pulse reflection time from the cementing plug can be clearly seen, and the cementing plug movement can be tracked in real time until it reaches the landing collar at job time equal 2450 s 1104.

[0053] To translate the reflection time into the position of the cementing plug in the wellbore, the velocity of pressure pulse propagation in the fluid media between the pressure transducer and top cementing plug was obtained experimentally. The moment of well bleed-off after the cementing plug set on the landing collar was used as it also resulted in the generation of a pressure pulse. A reflective signal intensity diagram was built after cepstral analysis of the pressure data near the moment of pressure release (FIG. 12). As a result, a distinct spot 1201 on the diagram was obtained. It corresponds to the reflection time from the top wiper plug setting on the landing collar1.01 s. Taking into account the known depth of the landing collar, the velocity of pressure pulse propagation in the displacement fluid (oil-base mud) was calculated as 1158 m/s. Using this result, the reflection time of the pressure pulse from the cementing plug can be translated to wiper plug position at any time when the reflection is distinguishable on the reflective signal intensity diagram.

[0054] Although only a few example embodiments have been described in detail above, those skilled in the art will readily appreciate that many modifications are possible in the example embodiments without materially departing from this invention. Accordingly, all such modifications are intended to be included within the scope of this disclosure as defined in the following claims.